Measuring an Event — Question 1

Section 37-2 · Physics pages 6052–6053

Question 1 A reception timestamp must be corrected for propagation A fixed detector at the origin receives a flash at tR = 12.0 µs from a known event position xE = 900 m. Use c = 3.00 × 108 m/s and Einstein-synchronized laboratory clocks. x ct E R Spacetime sketch; the vertical coordinate is ct. Labels specify events and worldlines. (a) Assign the emission event its laboratory time. (b) Find the timing error if reception is mistaken for emission, and write the general correction for either sign of xE.
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Question 1 - Solution A reception timestamp must be corrected for propagation x ct E R (a) Method and calculation tR = tE + |xE|/c. tE = 12.0 −3.0 = 9.0 µs . (b) Interpretation and further calculation tR −tE = 3.0 µs . tE = tR −|xE|/c . Physical check An event coordinate is an assigned emission time, not the time its image reaches a distant observer.

Question 1

A reception timestamp must be corrected for propagation

A fixed detector at the origin receives a flash at tR=12.0μst_R=12.0\,\mu\mathrm s from a known event position xE=900mx_E=900\,\mathrm m. Use c=3.00×108m/sc=3.00\times10^8\,\mathrm{m/s} and Einstein-synchronized laboratory clocks.

Diagram shown in the original SVG worksheet.

  1. Assign the emission event its laboratory time.

  2. Find the timing error if reception is mistaken for emission, and write the general correction for either sign of xEx_E.

Question 1 - Solution

A reception timestamp must be corrected for propagation

Diagram shown in the original SVG worksheet.

(a) Method and calculation

tR=tE+|xE|/c.t_R=t_E+|x_E|/c.tE=12.0−3.0=9.0μs.\boxed{t_E=12.0-3.0=9.0\,\mu\mathrm s}.

(b) Interpretation and further calculation

tR−tE=3.0μs.\boxed{t_R-t_E=3.0\,\mu\mathrm s}.tE=tR−|xE|/c.\boxed{t_E=t_R-|x_E|/c}.

Physical check

An event coordinate is an assigned emission time, not the time its image reaches a distant observer.